|
[1] Wan Y, Li J, Liu Y, et al. Overview of the present
progress and activities on the CFETR [J]. Nucl. Fusion,
2017, 57(10): 102009.
[2] Chen Jiale, Chan Vincent S, Jian Xiang, et al. Integrated
modeling of CFETR hybrid scenario plasmas [J]. Nucl.
Fusion, 2021, 61: 046002.
[3] Fujita T, Ide S, Kamada Y, et al. Quasisteady
high-confinement reversed shear plasma with large
bootstrap current fraction under full noninductive current
drive condition in JT-60U [J]. Physical review letters,
2001, 87(8): 085001.
[4] Litaudon X, Crisanti F, Alper B, et al. Towards fully
non-inductive current drive operation in JET [J]. Plasma
Phys. Contr. F., 2002, 44(7): 1057.
[5] Shimada M, Campbell D, Mukhovatov V, et al. Chapter 1:
Overview and summary [J]. Nucl. Fusion, 2007, 47(6):
S1.
[6] Gormezano C, Sips A C C, Luce T C, et al. Chapter7:
Steady state operation [J]. Nucl. Fusion, 2007, 47(6):
S285.
[7] Artaud J F, Imbeaux F, Garcia J, et al. METIS: A fast
integrated tokamak modelling tool for scenario design [J].
Nucl. Fusion, 2018, 58(10): 105001.
[8] Houlberg W A, Gormezano C, Artaud J F, et al.
Integrated modelling of the current profile in steady state
and hybrid ITER scenarios [J]. Nucl. Fusion, 2005,
45(11): 1309.
[9] Besseghir K, Garcia J, Artaud J F, et al. Achieving and
sustaining advanced scenarios in ITER modelled by
CRONOS and DINA-CH [J]. Plasma Phys. Contr. F.,
2013, 55: 125012.
[10] Garcia J, Giruzzi G, Artaud J F, et al. Analysis of DEMO
scenarios with the CRONOS suite of codes [J]. Nucl.
Fusion, 2008, 48: 075007.
|
